Methods for eliminating error sources of magnetic sensors used for the measurement of coating thickness

ABSTRACT

The invention relates to a method which allows to compensate errors due to offset voltages and external magnetic fields when using a magnetic sensor for coating thickness measurement. Also a method is described which allows compensation of a temperature dependent change of the output voltage of the magnetic sensor.

FIELD OF THE INVENTION

[0001] The invention relates to a method to measure non-magnetic coatings on ferro-magnetic substrates, using a magnetic sensor, where errors due to offset voltage of the magnetic sensor, temperature dependence of the sensor parameters and disturbing magnetic fields are compensated.

DESCRIPTION OF THE PRIOR ART

[0002] Patent EP0028487 discloses a measuring device that uses a Hall-sensor together with a permanent magnet. In this device the flux of external magnetic fields is superimposed to the flux of the internal permanent magnet and can not be separated. Therefore the change of the output signal of the Hall-sensor due to these external fields can not be determined. This results in erroneous measurements.

[0003] Pat. DE19910411 discloses a method for offset compensation of Hall-sensors. This method eliminates the offset by applying two different currents to the Hall-sensor, measuring the Hall-voltage at each current and calculating the offset from these two measured voltages. However this method does not allow for compensation of external magnetic fields.

[0004] In Pat. U.S. Pat. No. 33,359,495 a device is described that has a Hall-sensor with a coil arranged around the Hall-sensor. This device uses alternating electromagnetic fields generating eddy currents in the substrate. These eddy currents strongly depend on the conductivity of the substrate. The eddy currents in turn generate a secondary magnetic field opposed and superimposed to the primary field. This results in a change of the output voltage of the Hall-sensor. Since the strength of the eddy currents and consequently the strength of the secondary magnetic field strongly depend on the conductivity, this has a negative influence on the measuring results. An additional error occurs when the substrate is covered with a conductive coating. Also in the conductive coating eddy currents are generated. They have the same effect on the flux through the Hall-sensor as those generated in the substrate.

SUMMARY OF THE INVENTION

[0005] It is an object of the invention to provide simple methods which allow to eliminate the different error sources when using magnetic sensors for the measurement of coating thickness.

[0006] With the first two methods the influence of external magnetic fields, as they can be present in mechanically or thermally treated substrates, or of time varying fields on the measuring device can be eliminated. Additionally this invention makes use of the advantages of the static magnetic field being insensitive to the conductivity of substrate and metal coatings.

[0007] A further advantage of this method is the automatic compensation of the temperature dependent offset voltage of magnetic sensors. This offset voltage occurs when applying a current to the sensor, even in the absence of a magnetic field.

[0008] A further described method of this invention can be used to compensate the influence of temperature on the signal voltage.

BRIEF DESCRIPTION OF THE DRAWINGS

[0009]FIG. 1 is a block diagram of the measuring device.

[0010]FIG. 2 is a circuitry block diagram of the magnetic sensor for compensation of the temperature dependence of the signal voltage.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

[0011] The measuring device is equipped with a magnetic sensor 10 and a coil 20 disposed in the neighbourhood of the sensor. The control unit 30 contains the sensor electronics 31 to feed the magnetic sensor 10 with a current I and to receive the signal voltage U. The control unit 30 also contains the coil control unit 32 to feed the current I_(c) through the coil 20.

[0012] The compensation of external magnetic fields as well as the offset voltage of the magnetic sensor 10 can be performed by either of the methods described as preferred embodiments hereafter.

[0013] With the first method the output voltage U in the magnetic sensor 10 is measured first by the magnetic sensor control unit 31 without a current I_(c) through the coil 20, when the measuring probe 15 is placed on the object under test 50. The output voltage U depends on the external magnetic field B_(ext) through the magnetic sensor 10. This output voltage U₁, is transferred from the control unit 30 to the evaluation unit 40. There it is digitised and stored. With the next step a current I_(c) is feed through the coil 20. This current generates a magnetic field B that is superimposed to the external magnetic field B_(ext). This creates a different magnetic flux through the magnetic sensor 10 and consequently a different output voltage U₂. This voltage U₂ is transferred from the control unit 30 to the evaluation unit 40. There it is digitised and stored. A linear relation exists between output voltage U and magnetic flux B through the magnetic sensor which can be written in the following form:

U=U ₀ +K·B·I  (1)

[0014] U₀ is the offset voltage, K is the sensor constant and I is the current through the magnetic sensor 10. Equation 1 immediately shows that the output voltage is the sum of the offset voltage and the sum of all magnetic flux components B_(a), B_(b), . . . through the magnetic sensor 10:

U=U ₀ +U _(a) +U _(b) + . . . =U ₀ +K·(B _(a) +B _(b)+ . . . )·I  (2)

[0015] Therefore in the evaluation unit 40 the following difference can be calculated:

U _(res)=(U ₂ −U ₁)=[U _(o) +K·(B+B _(ext))·I]−[U _(o) +K·B _(ext) ·I]=K·B·I  (3)

[0016] The result U_(res) represents the voltage the magnetic sensor would generate if no external magnetic field were present. Simultaneously the offset voltage U₀ is eliminated. Using the functional relation between output voltage U of the magnetic sensor 10 and the distance of the sensor from the substrate (=coating thickness d=f(U)) the true coating thickness d can be calculated from the result U_(res).

[0017] With the second method a certain current I_(C1) is feed through the coil 20 by the coil control unit 32 when the measuring probe is placed on the object under test. The magnetic field B₁ generated by this current, together with an external magnetic field B_(ext), generates a magnetic flux through the magnetic sensor 10, resulting in an output voltage.

U ₁ =U ₀ +K·(B ₁ +B _(ext))·I  (4)

[0018] This output voltage U₁ is transferred from the control unit 30 to the evaluation unit 40. There it is digitised and stored. With the next step a second current I_(C2) is feed through the coil 20. In a preferred embodiment the current is selected as I_(C2)=−I_(C1). The absolute value of the magnetic field B₂ is the same as that of B₁, but with reverse polarity: B₂=−B₁. The magnetic field B₂, together with the external magnetic field B_(ext) generates a magnetic flux through the magnetic sensor 10, resulting in an output voltage:

U ₂ =U ₀ +K·(B ₂ +B _(ext))·I=U ₀ +K·(−B ₁ +B _(ext))·I  (5)

[0019] This output voltage U₂ is transferred from the control unit 30 to the evaluation unit 40. There it is digitised and stored. Using equation 2 and the two digitised output voltages U₁ and U₂, the voltage resulting from the external magnetic field B_(ext) and the offset voltage U₀ can be eliminated as follows:

U _(res) =[U ₁ −U ₂ ]=K·[(B ₁ +B _(ext))−(B ₂ +B _(ext))]·I=K·[B ₁ −B ₂ ]·I  (6)

[0020] Because of B₂=−B₁, =B equation 6 can be rewritten as:

U _(res)=2·K·B ·I  (7)

[0021] Using the functional relation between output voltage U of the magnetic sensor 10 and the distance of the sensor from the substrate (=coating thickness d=f(U)) the true coating thickness d can be calculated from the result U_(res).

[0022] In a preferred embodiment the influence of time varying magnetic fields, which usually have typical frequencies such as 60 Hz (e.g. those generated by transformers), can be eliminated by repeated changes between those two currents I_(C1) and I_(C2). The resulting output voltage is determined using the following equation:

U _(res) ={[U ₁ −U ₂]₁ +[U ₁ −U ₂]₂ + . . . +[U ₁ −U ₂]_(N) }/N =K·{[(B ₁ +B _(ext1))−(B ₂ +B _(ext2))]₁+[(B ₁ +B _(ext1))−(B ₂ +B _(ext2))]₂+ . . . +[(B ₁ +B _(ext1))−(B ₂ +B _(ext2))]N}/N·I =2 K·[B+{(B _(ext1) −B _(ext2))₁+(B _(ext1) −B _(ext2))₂+ . . . +(B _(ext1) −B _(ext2))_(1N) }/N]·I  (8)

[0023] with N being the number of repetitions. Those components of external magnetic fields in curved brackets will be averaged to zero, especially when the N pairs of measurements are taken in an interval that which is equal to one or several periods of the time varying magnetic field.

[0024] A further method in accordance with this invention allows to compensate the temperature dependence of the output voltage U. The temperature in the magnetic sensor 10 or the temperature change with respect to a reference temperature can be determined by measuring the internal resistance 11 of the magnetic sensor 10. This can be used to determine a compensation factor to correct the output voltage for temperature changes.

[0025] Starting from equation 1 the temperature gradient of th output voltage can be calculated as follows (a change in offset voltage can be neglected as effect of second order):

dU/dT=B·[dK _(H) /dT·I+K·dI/dT]=B·K·I·[α+β]  (9)

[0026] using the following abbreviations:

dK/dT=K(T ₀)·α, dI/dT=I(T ₀)·β

[0027] K(T₀) und I(T₀) are related to reference temperature T₀.

[0028] α and β are the temperature coefficients of the output voltage U and the sensor resistance 11 respectively. Since the coefficients α and β are known for each individual type of magnetic sensor, these parameters can be implemented directly in the control unit or used as parameters in a digital control unit.

[0029] The temperature dependant output voltage can be determined using the following equation:

U(T)=U(T ₀)+dU/dT·(T−T ₀)=B·K(T ₀)·I(T ₀)·{1+[α+β]·(T−T ₀)}  (10)

[0030] Equation 10 shows that the output voltage, measured at a temperature T, needs to be corrected by a factor {1+[α+β]·(T−T₀)} as given in equation 10, in order to reduce the output voltage to the correct value at reference temperature T₀. To do so the evaluation unit 40 has to calculate the factor in curved brackets which is transferred via the control unit 30 to the control of the magnetic sensor 31 to adjust the current I through the magnetic sensor by this factor.

[0031] To determine the temperature T the voltage drop across the sensor resistance 11 is measured by the sensor control unit 31 by feeding a constant current through this resistance 11. First this is done at temperature T₀ as a reference, and then at each measurement of the output voltage U. To calculate the actual temperature T or the temperature deviation ΔT from the reference temperature T₀ the following equation is used:

R(T)=R(T ₀)·[1+β·(T−T ₀)]=R(T ₀)·[1+β·ΔT]  (11)

[0032] β is the temperature coefficient of the sensor resistance 11 given above.

[0033] Then the temperature difference relative to T₀ is calculated as:

ΔT=(1/β)·R(T)/R(T ₀)  (12)

[0034] The procedure to determine a temperature compensated coating thickness is as follows:

[0035] First with a reference measurement the sensor resistance R(T₀) is determined in the control unit 30. This value is digitised and store in the evaluation unit 40. Each time a coating thickness measurement is taken the value R(T) is determined first, transferred from the control unit 30 to the evaluation unit 40, where it is digitised and stored. This value is then used to calculate the temperature difference ΔT according to equation 12. Subsequently, using ΔT, the correction factor {1+[α+β]·(T−T₀)} is calculated in the evaluation unit 40 and transferred to the control unit 30. Then this parameter is used in the magnetic sensor control unit 31 to adjust the current I such, that the output voltage conforms to the respective voltage at reference temperature T₀.

[0036] Alternatively to adjusting the current I through the resistor 11 of the magnetic sensor 10 upon temperature change the correction of the output voltage U at the measured temperature T can also be done digitally in the evaluation unit 40 using equation 10 and 12.

[0037] Of course it is obvious for a person skilled in the art to combine the method for temperature compensation of the output voltage with one of the methods for compensation of external magnetic fields. 

1. Method to determine the thickness of a coating on a ferro-magnetic substrate using a device having a magnetic sensor element and a coil, the method comprising the steps: measuring the output voltage of a magnetic sensor element generated by an external magnetic field; generating a magnetic field by applying a current to the coil and measuring the output voltage of the magnetic sensor element; the voltage measured in the first step is subtracted from the voltage measured in the second step; the difference is used to determine the coating thickness.
 2. Method to determine the thickness of a coating on a ferro-magnetic substrate using a device having a magnetic sensor element and a coil, the method comprising the steps: a magnetic field B₁, generated by the current I₁ in the coil, generates an output voltage U₁ in the magnetic sensor element, the output voltage depending on the distance of the magnetic sensor element from the substrate and on external magnetic fields; the control unit determines the output voltage U₁ of the magnetic sensor element generated in the first step; a second current I₂ through the coil and the resulting magnetic field B₂ generates a second output voltage U₂; the control unit determines the output voltage U2 of the magnetic sensor element generated in the third step; the evaluation unit determines the coating thickness from the difference of the two output voltages.
 3. The method of claim 2, wherein the current I₁, has the same absolute value as I₂, but is of opposite polarity.
 4. The method of claim 2, wherein the steps one through four are repeated several times.
 5. The method of claim 1 or 2, wherein the magnetic sensor element is a Hall-sensor element.
 6. The method of claim 1 or 2, wherein the magnetic sensor element is a GMR-sensor element.
 7. Method to compensate the temperature dependence of the signal in a measuring device for coating thickness using a magnetic sensor element as measuring device, wherein the resistance of the magnetic sensor element is determined to receive a temperature signal which is used, together with the temperature coefficients of the magnetic sensor element, to determine a factor to correct the output voltage so that the corrected value of the output voltage is related to a reference temperature.
 8. Method of claim 7, wherein the correction of the signal voltage is done by adjusting the current through the resistance of the magnetic sensor element.
 9. The method of claim 7, wherein the correction of the measured output voltage is performed by calculation.
 10. The method of claim 1, wherein the measurement of the output voltage is corrected with the method of any one of claims 7, 8 or
 9. 11. The method of claim 2, wherein the measurement of the output voltage is corrected with the method of any one of claims 7, 8 or
 9. 12. The method of claim 7, wherein the magnetic sensor is a Hall-sensor element.
 13. The method of claim 7, wherein the magnetic sensor is a GMR-sensor element. 